Light emitting device, light emitting device package, and lighting system including the same

ABSTRACT

A light emitting device, a light emitting device package, and a lighting system are provided. The light emitting device includes a first conductive type semiconductor layer, a second conductive type semiconductor layer, and an active layer between the first and second conductive type semiconductor layers. The active layer includes a first active layer adjacent to the second conductive type semiconductor layer, a second active layer adjacent to the first conductive type semiconductor layer, and a gate quantum barrier between the first and second active layers.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is a Continuation Application of U.S. patentapplication Ser. No. 13/177,766 filed on Jul. 7, 2011, now U.S. Pat. No.8,421,075 issued Apr. 16, 2013 which claims under 35 U.S.C. §119 toKorean Patent Application No. 10-2010-0066396(filed Jul 9, 2010),10-2010-0068122(filed Jul. 14, 2010) and 10-2010-0076758(filed Aug. 10,2010), which are hereby incorporated by references in their entireties.

BACKGROUND

The present disclosure relates to a light emitting device, a lightemitting device package, and a lighting system.

Light emitting devices based on a nitride semiconductor thin filmconvert electric energy into light energy. With the development ofthin-film growth techniques and light emitting materials, light emittingdevices, using a nitride semiconductor material which is formed bycombining the group III element and group V element of the periodictable, emit white light having various wavelengths (colors) such as red,green, blue, and ultraviolet light, and realize high efficient whitelight by using fluorescent materials or combining colors. Moreover,light emitting devices based on a nitride semiconductor thin film havelow power consumption, semipermanent life, fast response time,stability, and environmental friendliness compared to the existing lightsources such as fluorescent lamps and incandescent lamps. Therefore, theapplication of light emitting devices are being expanded to LightEmitting Diode (LED) backlights that replace Cold Cathode FluorescentLamps (CCFLs) configuring the backlight unit of a Liquid Crystal Display(LCD) device, white LED lighting devices for replacing fluorescent lampsor incandescent bulbs, the head lights of vehicles, traffic lights, etc.In expanding the application of nitride semiconductor light emittingdevices, technology for developing high efficient light emitting devicesis fundamentally required.

Nitride semiconductor light emitting devices of the related art have alimitation in that light emission efficiency is reduced due to a seriousnonradiative recombination loss process when a high current is injected.The cause is not clearly established, and many global scholars andexperts are actively researching for finding the cause. Also, nitridesemiconductor light emitting devices of the related art have alimitation in that light emission efficiency is reduced by anonradiative recombination loss process due to a crystal defect when alow current is injected.

In nitride semiconductor light emitting devices emitting blue light andgreen light, the reduction in light emission efficiency that is causedwhen injecting a high current is one of urgent technical limitations inimplementing light emitting devices for high output and high efficientlighting.

Consequently, it is acutely being required to develop ideal nitridesemiconductor light emitting device structures that provide excellentlight emitting quantum efficiency in all injection current regionsranging from a region having the low amount of injection current to aregion having the high amount of injection current.

SUMMARY

Embodiments provide a light emitting device, a light emitting devicepackage, and a lighting system, which innovatively solve the limitationsof the related art nitride semiconductor light emitting devices such asthe reduction in light emission efficiency due to nonradiativerecombination loss in injecting a high current and the reduction inlight emission efficiency that is caused by nonradiative recombinationloss due to a crystal defect in injecting a low current, therebyrealizing high efficient light emission characteristics in all injectioncurrent regions.

In one embodiment, a light emitting device includes: a first conductivetype semiconductor layer; a second conductive type semiconductor layer;and an active layer between the first and second conductive typesemiconductor layers, wherein the active layer includes: a first activelayer adjacent to the second conductive type semiconductor layer; asecond active layer adjacent to the first conductive type semiconductorlayer; and a gate quantum barrier between the first and second activelayers.

In another embodiment, a light emitting device includes: a firstconductive type semiconductor layer; a second conductive typesemiconductor layer; and an active layer between the first and secondconductive type semiconductor layers, wherein the active layer includes:a third active layer of a multiple-quantum well structure adjacent tothe first conductive type semiconductor layer; a fourth active layer ofa single quantum well structure adjacent to the second conductive typesemiconductor layer; and a gate quantum barrier between the third andfourth active layers.

In further another embodiment, a light emitting device package includesthe light emitting device; a package body in which the light emittingdevice is disposed; and one or more electrodes electrically connectedthe light emitting device and the package body.

In still further another embodiment, a lighting system includes a lightemitting unit including the light emitting device package.

The details of one or more embodiments are set forth in the accompanyingdrawings and the description below. Other features will be apparent fromthe description and drawings, and from the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 is a view schematically illustrating an active layer energy bandof a related art nitride semiconductor light emitting device including amultiple-quantum well structure active layer.

FIG. 2 is a characteristic view showing internal light emission quantumefficiency based on the increase in the injected current amount of arelated art nitride semiconductor light emitting device including amultiple-quantum well structure active layer (see FIG. 1).

FIG. 3 is a view schematically illustrating an active layer energy bandof a related art nitride semiconductor light emitting device includingan active layer of a wide single quantum well structure.

FIG. 4 is a characteristic view showing internal light emission quantumefficiency based on the increase in the injected current amount of arelated art nitride semiconductor light emitting device including anactive layer of a wide single quantum well structure (see FIG. 3).

FIG. 5 is an exemplary view illustrating a cross sectional surface of alight emitting device according to an embodiment.

FIG. 6 is a view schematically illustrating an energy band gap of anactive layer of a light emitting device including first and secondactive layers (i.e., dual active layer), in a light emitting deviceaccording to a first embodiment.

FIG. 7 is a characteristic view showing light emission efficiency basedon an injected current of a dual-active nitride semiconductor lightemitting device according to a first embodiment.

FIG. 8 is a view schematically illustrating an energy band gap of anactive layer of a dual-active light emitting device having a dual activelayer which includes a first active layer of a multiple-quantum wellstructure and a second active layer of a super lattice structure, in alight emitting device according to a second embodiment.

FIG. 9 is a view schematically illustrating an energy band gap of anactive layer of a light emitting device having a dual active layer whichincludes a first active layer of a narrow single quantum well structureand a second active layer of a wide single quantum well structure, in alight emitting device according to a third embodiment.

FIG. 10 is a view showing optical output power characteristic based onan injected current of a nitride semiconductor blue light emittingdevice including a dual active layer, in a light emitting deviceaccording to a third embodiment.

FIG. 11 is a view schematically illustrating an energy band gap of anitride semiconductor light emitting device including first and secondactive layers (i.e., dual active layer), in a light emitting deviceaccording to a fourth embodiment.

FIG. 12 is a view showing a distribution of electrons and holes inside adual active layer when a low current is injected into a light emittingdevice including the dual active layer, in a light emitting deviceaccording to a fourth embodiment.

FIG. 13 is a view showing a distribution of electrons and holes inside adual active layer when a high current is injected into a light emittingdevice including the dual active layer, in a light emitting deviceaccording to a fourth embodiment.

FIG. 14 is a view showing internal light emission quantum efficiencybased on an injected current density of a nitride semiconductor bluelight emitting device, in a light emitting device according to a fourthembodiment.

FIG. 15 is a view schematically illustrating an energy band gap of anactive layer of a light emitting device having a multiple-active layerwhich includes one first active layer of a multiple-quantum wellstructure and two second active layers of a wide single quantum wellstructure respectively disposed adjacently to an electron injectionlayer and a hole injection layer, in a light emitting device accordingto a fifth embodiment.

FIG. 16 is a view showing an optical output power of a nitridesemiconductor blue light emitting device, in a light emitting deviceaccording to a fifth embodiment.

FIG. 17 is a cross sectional view illustrating a light emitting devicepackage according to an embodiment.

FIG. 18 is a perspective view illustrating a lighting unit according toan embodiment.

FIG. 19 is a perspective view illustrating a backlight unit according toan embodiment.

DETAILED DESCRIPTION OF THE EMBODIMENTS

Reference will now be made in detail to the embodiments of the presentdisclosure, examples of which are illustrated in the accompanyingdrawings.

Hereinafter, a light emitting device, a light emitting device package,and a lighting system, according to embodiments, will be described indetail with reference to the accompanying drawings.

In the description of embodiments, it will be understood that when alayer (or film) is referred to as being ‘on’ another layer or substrate,it can be directly on another layer or substrate, or intervening layersmay also be present. Further, it will be understood that when a layer isreferred to as being ‘under’ another layer, it can be directly underanother layer, and one or more intervening layers may also be present.In addition, it will also be understood that when a layer is referred toas being ‘between’ two layers, it can be the only layer between the twolayers, or one or more intervening layers may also be present.

FIG. 1 is a view schematically illustrating an active layer energy bandof a related art nitride semiconductor light emitting device including amultiple-quantum well structure active layer. FIG. 2 is a characteristicview showing internal light emission quantum efficiency based on theincrease in the injected current amount of a related art nitridesemiconductor light emitting device including a multiple-quantum wellstructure active layer (see FIG. 1).

As shown in FIG. 2, a technology of manufacturing a related art nitridesemiconductor light emitting device based on a multiple-quantum wellstructure has a limitation in that light emission quantum efficiency issignificantly reduced in inverse proportion to the increase in aninjected current. In a nitride semiconductor multiple-quantum wellstructure active layer of the related art, electrons injected from anN-type GaN-based electron injection layer are disposed at quantizedenergy levels that are formed on a quantum well conduction band (Ec),and holes injected from an P-type GaN-based hole injection layer aredisposed at quantized energy levels that are formed under a quantum wellvalence band (Ev). Electrons and holes disposed at ground statequantized energy levels in a quantum well are combined to emit lightwhen a quantum-mechanical combination condition is satisfied.

A ground state (quantum number, n=1) quantized energy level having thelowest energy state in one quantum well may quantum-mechanically retainonly a certain amount of electrons or holes. An electron and a holedisposed at a higher quantized energy level (higher quantum number ofquantized energy level) are higher than an electron and a hole disposedat an energy state of a ground state. Therefore, when the number ofinjected electrons or holes is sufficient, carriers (electrons andholes) disposed at a high quantized energy level in one quantum wellmove to a ground state in another adjacent quantum well and participatein light emission.

In a related art nitride semiconductor light emitting device including amultiple-quantum well structure active layer (light emission layer),however, all quantum well layers in an active layer cannot conformallydistribute or accommodate a plurality of injected carriers, and only asmall number of quantum well layers adjacent to a hole injection layerparticipate in light emission. Therefore, when the amount of injectedcurrent is sufficient, surplus electrons and holes that are noteffectively confined are generated inside an active layer.

The surplus electrons or holes do not participate in light emission, andare self vanished in the active layer by an auger nonradiativerecombination process or leaked to outside the active layer.

The auger nonradiative recombination process is expressed as Cn³ (whereC is an auger constant, and n is an injected carrier density), and is afundamental attribute of a material that is generatedquantum-mechanically. Leakage to outside the active layer occurs as thequantum barrier overflow of an injected carrier.

In the related art nitride semiconductor light emitting device, a verylarge internal field fundamentally exists inside the active layer due tothe fundamental polar properties of a material, and also a seriouscarrier overflow occurs because an electron injected into the activelayer has hot carrier properties.

As a result, when an injected current increases, the nonradiative lossof electrons and holes is increased, and thus, the light emissionefficiency of the active layer, for example, internal quantum efficiencyis significantly decreased.

In the nitride semiconductor light emitting device based on themultiple-quantum well structure active layer, the reduction in lightemission efficiency that is caused when applying a high current is oneof urgent technical limitations in implementing light emitting devicesfor high output power lighting.

FIG. 3 is a view schematically illustrating an active layer energy bandof a related art nitride semiconductor light emitting device includingan active layer of a wide single quantum well structure.

FIG. 4 is a characteristic view showing internal light emission quantumefficiency based on the increase in the injected current amount of arelated art nitride semiconductor light emitting device including a widesingle quantum well structure active layer (see FIG. 3). As shown inFIG. 4, a technology of manufacturing a related art nitridesemiconductor light emitting device based on a wide single quantum wellstructure has a limitation in that light emission quantum efficiency issignificantly reduced by nonradiative loss due to a crystal defect in alow current region.

The related art nitride semiconductor light emitting device includes anInGaN single quantum well structure layer, having a relatively thickactive layer, as an active layer.

A relatively wide InGaN single quantum well structure active layer (seeFIG. 3) can effectively accommodate relatively many electrons and holescompared to the related art multiple-quantum well structure active layer(see FIG. 1). Accordingly, when the amount of injected current issufficient, the light emission efficiency of the active layer isexcellent.

However, a light emitting device using a semiconductor thin filmfundamentally has a nonradiative loss attribute due to a crystal defectexisting inside the active layer. Such crystal defect-relatedShockley-Read-Hall (SHR) nonradiative recombination process is expressedas “An” (where A is an SHR constant, and n is an injected carrierdensity), and is a dominant carrier recombination process in a lowinjection current region.

As a result, a nitride semiconductor light emitting device including arelatively thick single quantum well structure active layer is increasedrelatively in total number of crystal defects existing in an activelayer, and thus, a nonradiative loss effect due to the crystal defectsis increased. Therefore, the nitride semiconductor light emitting deviceincluding the relatively thick single quantum well structure activelayer has a limitation in that internal quantum efficiency (lightemission efficiency) of a device is very low in a low current injectionregion.

Consequently, the related art nitride semiconductor light emittingdevice based on a multiple-quantum well structure active layer hasexcellent light emission efficiency due to an efficient quantumconfinement effect in the low current injection region, but has very lowlight emission efficiency in a high current injection region. On theother hand, the related art nitride semiconductor light emitting devicebased on a relatively thick single quantum well structure active layerhas excellent light emission efficiency in the high current injectionregion, but has very low light emission efficiency in the low currentinjection region. Accordingly, an embodiment proposes an ideal nitridesemiconductor light emitting device structure that has excellent lightemission efficiency in both the low current injection region and thehigh current injection region.

In the nitride semiconductor light emitting device, carriers injectedfrom a carrier injection layer into an active layer perform one of thefollowing four processes.

Entire carrier recombination is “R=An+Bn²+Cn³+L(n), where n is aninjected carrier density, A is an SHR constant, B is a radiativerecombination constant, C is an auger constant, L is a carrier leakageprocess function depending on higher orders of n.

In the four carrier recombination processes, a light emission process isBn², and the other three processes are a crystal defect nonradiativeprocess, an auger nonradiative process, and a carrier leakagenonradiative process, respectively.

In order to maximize the internal quantum efficiency of the nitridesemiconductor light emitting device, therefore, the effect of the SHRprocess being a dominant nonradiative process may be minimized wheninjecting a low current, and the effects of the auger process andcarrier leakage process being a dominant nonradiative process may beminimized when injecting a high current.

According to an approach for realizing an embodiment, a quantumconfinement effect may be maximized by minimizing a light emission areawhen injecting a low current, and the light emission area may bemaximized when injecting a high current.

According to an embodiment, an active layer structure included in onelight emitting device may be a variable multi-functional structureaccording to an injection current region. According to an embodiment, asone embodiment for realizing a variable multi-functional active layerstructure, a dual active layer concept is proposed as follows.

According to an embodiment, the dual (or multiple) active layer conceptincludes a first active layer that serves as a main layer in a lowcurrent region, a second active layer that serves as a main layer in ahigh current region, and a gate quantum barrier between the first andsecond active layers, and realizes high LED light emission efficiency inall injection current regions ranging from the low current region to thehigh current region. According to an embodiment, functions of mainelements are as follows.

The first active layer has a quantum well structure, and thus maximizeslight emission efficiency due to the limit of a light emission area anda quantum confinement effect, in a the low current region. The firstactive layer includes a relatively thin quantum well layer, allows asmall number of quantum well layers to participate in light emission,and thus minimizes the SHR nonradiative recombination process due to acrystal defect.

The gate quantum barrier controls the quantum-mechanical tunneling anddrift transport attributes of carriers to allow the second active layerto mainly participate in light emission, at a certain injection currentor higher. According to an embodiment, the gate quantum barrier isdisposed between the first and second active layers having a quantumwell structure, and may vary the thickness of the gate quantum barrierand the size of the energy band gap to control the amount of criticalinjection current at which the second active layer start participatingin light emission.

The second active layer has a structure that accommodates many carriers,and serves as a main active layer having excellent light emissionefficiency in the high current region.

According to an embodiment, for example, by including a thin quantumbarrier, the second active layer structure may have a super latticestructure that may form a mini-energy band through quantum-mechanicaltunneling, a relatively wide single quantum well structure, or arelatively wide multiple-quantum well structure.

The super lattice structure, the relatively wide single quantum wellstructure, or the relatively wide multiple-quantum well structureeffectively accommodates many carriers to allow the carriers toparticipate in light emission when injecting a high current, therebyrealizing excellent light emission efficiency characteristic in the highcurrent region.

According to an embodiment, a main difference between the first andsecond active layers is that the second active layer has aquantum-mechanically quantized density of state higher than that of thefirst active layer. The second active layer has a relatively higherdensity of state, and thus can effectively accommodate more carriersinto a light emission layer than the first active layer.

A wavelength emitted from an active layer of a light emitting device isquantum-mechanically determined according to the width (thickness) of aquantum well layer and the size of an energy band gap. Therefore, thesize of the energy band gap of the quantum well layer may beappropriately controlled in order for the second active layer to emitlight of a wavelength equal or similar to that of the first activelayer.

Wavelengths of two active layers (i.e., the first and second activelayers) may be equal or similar for implementing one light emittingdevice that emits light of single color with good color purity or thesame wavelength.

For example, when the light of the first active layer and the light ofthe second active layer are expressed as color coordinates, a straightline joining the color coordinate of the first active layer and thecolor coordinate of the second active layer may be positioned in a samecolor area including the color coordinates of the two active layers.Also, light emitted from each of the first and second active layers mayhave color purity of 80% or higher.

According to an embodiment, when the first active layer that mainlyperforms a function in the low current region is included adjacently toa hole injection layer, the size of an energy band gap of a quantum wellin the first active layer may be equal to or greater than that of anenergy band gap of a quantum well in the second active layer. FIG. 5 isa cross sectional view exemplarily illustrating a light emitting device100 according to an embodiment.

In an embodiment, a vertical light emitting device is mainly described,but is merely an example. An embodiment may be applied to horizontallight emitting devices, flip-chip light emitting devices, and hybridlight emitting devices including a via hole.

The light emitting device 100 according to an embodiment may include alight emitting structure, a second electrode layer 140 formed under thesecond conductive type semiconductor layer 130, and a first electrode150 on the first conductive type semiconductor layer 110. Herein, thelight emitting structure includes a first conductive type semiconductorlayer 110, an active layer 120, and a second conductive typesemiconductor layer 130.

The first conductive type semiconductor layer 110 may be formed of agroup III-V compound semiconductor doped with a first conductive dopant.When the first conductive type semiconductor layer 110 is an N-typesemiconductor layer, the first conductive dopant as an N-type dopant mayinclude Si, Ge, Sn, Se, or Te, but the present disclosure is not limitedthereto.

The first conductive type semiconductor layer 110 may include asemiconductor material having a compositional formula ofIn_(x)Al_(y)Ga_(1-x-y)N (0≦x≦1, 0≦y≦1, 0≦x+y≦1).

The first conductive type semiconductor layer 110 may be formed of atleast one of GaN, InN, AlN, InGaN, AlGaN, InAlGaN, AlInN, AlGaAs,InGaAs, AlInGaAs, GaP, AlGaP, InGaP, AlInGaP, and InP.

The active layer 120 may include a first active layer 121 thateffectively performs a function in the low current region, a secondactive layer 122 that effectively performs a function in the highcurrent region, and a gate quantum barrier 125 between the first andsecond active layers 121 and 122, but is not limited thereto. The activelayer 120 will be specifically described in the following embodiment.

The second conductive type semiconductor layer 130 may include a groupIII-V compound semiconductor that is doped with a second conductivedopant, for example, include a semiconductor material having acompositional formula of In_(x)Al_(y)Ga_(1-x-y)N (0≦x≦1, 0≦y≦1,0≦x+y≦1). For example, the second conductive type semiconductor layer130 may be formed of at least one material selected from among GaN, AlN,AlGaN, InGaN, InN, InAlGaN, AlInN, AlGaAs, GaP, GaAs, GaAsP, andAlGaInP. When the second conductive type semiconductor layer 130 is aP-type semiconductor layer, the second conductive dopant as a P-typedopant may include Mg, Zn, Ca, Sr, Ba, or the like. The secondconductive type semiconductor layer 130 may be formed as a single layeror a multi-layer, but the present disclosure is not limited thereto.

In an embodiment, the first conductive type semiconductor layer 110 maybe implemented as an N-type semiconductor layer, and the secondconductive type semiconductor layer 130 may be implemented as a P-typesemiconductor layer, but the present disclosure is not limited thereto.Also, a semiconductor layer having polarity opposite to that of thesecond conductive type semiconductor layer 130, for example, an N-typesemiconductor layer (not shown) may be formed on the second conductivetype semiconductor layer 130. Accordingly, the light emitting structuremay be implemented as one of an N-P junction structure, a P-N junctionstructure, an N-P-N junction structure, and a P-N-P junction structure.

The second electrode layer 140 may include a coupling layer 142, anohmic layer 144, a reflective layer 146, and a conductive supportsubstrate 148.

For example, the coupling layer 142 may include at least one of Ti, Au,Sn, Ni, Cr, Ga, In, Bi, Cu, Ag, and Ta.

For example, the ohmic layer 144 may be formed of at least one of indiumtin oxide (ITO), indium zinc oxide (IZO), indium zinc tin oxide (IZTO),indium aluminum zinc oxide (IAZO), indium gallium zinc oxide (IGZO),indium gallium tin oxide (IGTO), aluminum zinc oxide (AZO), antimony tinoxide (ATO), gallium zinc oxide (GZO), IZO nitride (IZON), Al—Ga ZnO(AGZO), In—Ga ZnO (IGZO), ZnO, IrOx, RuOx, NiO, RuOx/ITO, Ni/IrOx/Au,Ni/IrOx/Au/ITO, Ag, Ni, Cr, Ti, Al, Rh, Pd, Ir, Ru, Mg, Zn, Pt, Au, andHf, but the present disclosure is not limited thereto.

Moreover, the reflective layer 146 reflects light incident from thelight emitting structure, thereby improving the light extractionefficiency.

The reflective layer 146 may be formed of a metal or alloy including atleast one of Ag, Ni, Al, Rh, Pd, Ir, Ru, Mg, Zn, Pt, Au, and Hf. Also,the reflective layer 146 may be formed in a multi-layer including themetal or alloy and a light-transmitting conductive material such as IZO,IZTO, IAZO, IGZO, IGTO, AZO, and ATO. For example, the reflective layer146 may be formed in a stacked structure such as IZO/Ni, AZO/Ag,IZO/Ag/Ni, AZO/Ag/Ni.

The conductive support substrate 148 may support the light emittingstructure and supply a power to the light emitting structure. Theconductive support substrate 148 may be formed of a metal, a metalalloy, or a conductive type semiconductor material, which has highelectric conductivity.

For example, the conductive support substrate 148 may include at leastone of copper (Cu), copper alloy, gold (Au), nickel (Ni), molybdenum(Mo), copper-tungsten (Cu—W), and a carrier wafer (for example, Si, Ge,GaAs, GaN, ZnO, SiGe, SiC, or the like).

An electrochemical metal deposition method, a plating method, or abonding method using a eutectic metal may be used as a method of formingthe conductive support substrate 148.

Hereinafter, in embodiments, mechanisms of main elements in an epitaxialstructure (hereinafter referred to as an epi structure) will bedescribed in more detail by using some structural examples below.

(First epi Structure)

An epi structure according to a first structural example may be formedin the order of an electron injection layer/second active layer/gatequantum barrier/first active layer/hole injection layer

In the first structural example, when injecting a low current, carriersare mainly inputted into the first active layer to emit light. An energyband gap of the first active layer may be equal or similar to that ofthe second active layer. When the amount of injected current isincreased to higher than a certain amount of current, holes pass overthe gate quantum barrier and begin filling the second active layer.Therefore, when injecting a high current, the first and second activelayers participate in light emission, in which case the second activelayer having a greater capacity of accommodating carriers than the firstactive layer becomes a main light emitting source.

(Second epi Structure)

An epi structure according to a second structural example may be formedin the order of an electron injection layer/third active layer/gatequantum barrier/fourth active layer/hole injection layer.

In the second structural example, when injecting a low current, carriersare mainly inputted into the third active layer to emit light. An energyband gap of the fourth active layer may be greater than that of thesecond active layer. An energy band gap of the gate quantum barrier maybe less than that of the hole injection layer such that holes areeffectively injected into the third active layer when injecting a lowcurrent. When injecting a high current, electrons fill the third activelayer having a relatively less energy band gap, pass over the gatequantum barrier, and are injected into the fourth active layer toparticipate in light emission.

(Third epi Structure)

An epi structure according to a third structural example may be formedin the order of an electron injection layer/fourth active layer/gatequantum barrier/third active layer/gate quantum barrier/fourth activelayer/hole injection layer. In the third epi structure, when injecting alow current, carriers are mainly inputted into the third active layer toemit light. An energy band gap of the fourth active layer may be greaterthan that of the third active layer. An energy band gap of the gatequantum barrier may be less than that of the hole injection layer suchthat holes are effectively injected into the third active layer wheninjecting a low current.

When injecting a high current, electrons fill the third active layerhaving a relatively less energy band gap, drift-transport the gatequantum barrier, and are injected into the fourth active layer adjacentto the hole injection layer to participate in light emission. Wheninjecting a high current, holes fill the third active layer,drift-transport the gate quantum barrier, and are injected into thefourth active layer to participate in light emission.

An innovation point of an embodiment is to propose an intelligent smartlight emitting structure that overcomes the fundamental/structurallimits of the related art nitride semiconductor light emitting deviceincluding a single active layer.

The related art light emitting device based on a nitride semiconductorthin film, emitting a single color (i.e., single wavelength), includesone active layer in a thin film. The related art light emitting devicebased on a nitride semiconductor thin film, emitting dual colors ortriple colors (i.e., multiple wavelengths), includes two or three activelayers in a thin film.

However, such multiple-wavelength light emitting device is technologythat simultaneously emits blue light and green light, or blue light,green light and red light, and thus realizes white LED without using afluorescent material. An intelligent active layer structure including amultiple active layer, according to an embodiment, enables the nitridesemiconductor light emitting device emitting a single color (i.e.,single wavelength) to realize excellent light emission efficiency in allinjection current regions ranging from a low injection current region toa high injection current region, and thus has a differentiated point byproviding a concept that can overcome the fundamental limit of therelated art nitride semiconductor light emitting device technology.

Hereinafter, a light emitting device, a light emitting device package,and a lighting system, according to embodiments, will be described indetail for each embodiment.

<First Embodiment>

FIG. 6 is a view schematically illustrating an energy band gap of anactive layer of a light emitting device including a dual active layerbased on the first epi structure, in a light emitting device accordingto a first embodiment. In the first embodiment, the second active layermay have a super lattice structure, and the first active layer may havea single quantum well structure.

A light emitting device 100 according to the first embodiment mayinclude a first conductive type semiconductor layer 110, a secondconductive type semiconductor layer 130, and an active layer 120 betweenthe first and second conductive type semiconductor layers 110 and 130.The first conductive type semiconductor layer 110 may be an electroninjection layer, and the second conductive type semiconductor layer 130may be a hole injection layer. However, the present disclosure is notlimited thereto.

The active layer 120 may include a first active layer 121 adjacent tothe second conductive type semiconductor layer 130, a second activelayer 122 adjacent to the first conductive type semiconductor layer 110,and a gate quantum barrier 125 between the first and second activelayers 121 and 122.

In the light emitting structure according to the first embodiment, theactive layer 120 may include the first active layer 121 having a singlequantum well structure that effectively performs a function in the lowcurrent region, the second active layer 122 having a super latticestructure that effectively performs a function in the high currentregion, and the gate quantum barrier 125 between the first and secondactive layers 121 and 122.

In the light emitting structure according to the first embodiment, inimplementing the active layer 120, a light emitting region related tolight emission may be minimally designed with a quantum well structurein order to solve the reduction in light emission efficiency due to acrystal defect when injecting a low current, and a light emitting regionrelated to light emission may be maximally designed with a super latticestructure when injecting a high current.

In the first embodiment, the low current may be about 5 A/cm² or less,and the high current may be about 35 A/cm² or higher. However, thepresent disclosure is not limited thereto.

The first active layer 121 includes a quantum well including a quantizedenergy level that is formed quantum-mechanically. In the first activelayer 121, for convenience, n schematically indicates the quantum numberof quantized energy level where holes and electrons are placed in aquantum well showing a quantum effect.

The second active layer 122 is a light emission layer having a superlattice structure. In the multiple-quantum well structure of the secondactive layer 122, a quantum barrier may no longer show a quantumconfinement effect when the quantum barrier is sufficiently thin, andelectrons or holes confined in the quantum well pass through the thinquantum barrier by a quantum-mechanical tunneling effect and form aspecific mini-energy band by spreading into an entire super lattice. Inthe first embodiment, the band structure may be called a super latticemini-band, but the present disclosure is not limited thereto.

In this embodiment, the super lattice structure of the second activelayer 122 is a light emission region emitting light, and isdifferentiated from that the related art super lattice structure formoderating stress or injecting carriers is not a light emission region.

The second active layer 122 may include a plurality of multiple-quantumwell structures 122 a to 122 d and a multiple quantum (not shown), andthe quantum barrier of the second active layer 122 enables thequantum-mechanical tunneling of carriers (electrons or holes).

For example, the quantum barrier of the second active layer 122 may havea thickness d2 from about 0.2 nm to about 7 nm. For example, in thesuper lattice structure of the second active layer 122, an effectivemini-band may be formed when the thickness of the quantum barrier isabout 7 mm or less, and injected holes may be effectively distributedinto an entire super lattice.

Each of the quantum wells 122 a to 122 d of the second active layer 122may have a thickness of about 2 nm to about 10 nm, but the presentdisclosure is not limited thereto.

In this embodiment, when a low current is applied, the gate quantumbarrier 125 may confine a hole, injected into the first active layer 121through the second conductive type semiconductor layer 130, such thatthe injected hole cannot be transferred to the second active layer 122.When a high current equal to or higher than a certain injection currentis applied, the gate quantum barrier 125 may allow a hole, injected intothe first active layer 121 through the second conductive typesemiconductor layer 130, to be effectively transferred to the secondactive layer 122 through drift-transport.

For example, a thickness dg of the gate quantum barrier 125 may be about3 nm to about 15 nm. In a case where the gate quantum barrier 125 has athickness of less than about 3 nm, holes may not effectively be confinedin the quantum well of the first active layer 121 when a low current isinjected. In a case where the gate quantum barrier 125 has a thicknessof greater than about 15 nm, holes may not effectively pass over thegate quantum barrier 125 when a high current is injected

For example, the thickness dg of the gate quantum barrier 125 may beabout 4 nm to about 12 nm, but the present disclosure is not limitedthereto. In a case where the gate quantum barrier 125 has a thickness ofabout 4 nm or greater, holes may more effectively be confined in thequantum well of the first active layer 121 when a low current isinjected. In a case where the gate quantum barrier 125 has a thicknessof about 12 nm or less, holes may more effectively pass over the gatequantum barrier 125 and be injected into the second active layer 122when a high current is injected.

The size of the energy band gap of the gate quantum barrier 125 may begreater than that of the energy band gap of the quantum well in thefirst active layer 121, and be equal to or less than that of the energyband gap of the second conductive type semiconductor layer 130. When alow current is injected, the size of the energy band gap of the gatequantum barrier 125 may be greater than that of the energy band gap ofthe quantum well in the first active layer 121 in order to effectivelyconfine holes in the quantum well of the first active layer 121.

As an injected current increases, the number of holes accumulated intothe quantum well of the first active layer 121 increases, and a portionof holes is vanished by emitting light in combination of electrons.

When a high current is injected, holes may more effectively pass overthe gate quantum barrier 125 and be injected into the second activelayer 122, for which the size of the energy band gap of the gate quantumbarrier 125 may be less than that of the energy band gap of the quantumwell 121 in the second conductive type semiconductor layer 130. Theenergy band gap of the gate quantum barrier 125 may be changed bycontrolling the composition of a nitride semiconductor(In_(z)Al_(y)Ga_(1-x-y)N, 0≦x, y≦1) gate quantum barrier.

In this embodiment, the main mechanism of the ideal active layer 120uses the unique attributes of nitride semiconductor materials whereelectrons in the nitride semiconductor active layer 120 have loweffective mass and high mobility, and holes in the nitride semiconductoractive layer 120 have relatively higher effective mass and very lowmobility.

When a low current is injected, electrons injected from the firstconductive type semiconductor layer 110 (for example, an electroninjection layer) into the active layer 120 may easily pass over thesecond active layer 122 having a super lattice structure and the gatequantum barrier 125 and reach the quantum well layer of the first activelayer 121 because the electrons have relatively high mobility in theactive layer 120.

When a low current is injected, holes injected from the secondconductive type semiconductor layer 130 (for example, a hole injectionlayer) into the active layer 120 may be quantum-mechanically confined inthe quantum well of the first active layer 121 adjacent to the holeinjection layer and not effectively pass over the gate quantum barrier125 because the holes have high effective mass and low mobility.

On the other hand, when a high current is injected, holes injected fromthe hole injection layer into the active layer fill all the quantumwells of the first active layer 121, and then, surplus holes pass overthe gate quantum barrier 125 and reach the second active layer 122 of asuper lattice structure. The second active layer 122 may effectivelyaccommodate a lot of surplus holes, and by participating in lightemission, the second active layer 122 serves as a main active layer whena high current is injected. When a high current is injected, electronsinjected from the electron injection layer into the active layer may beeasily distributed in the entire active layer.

Mechanism of this embodiment will be described below in more detail withreference to FIG. 6.

When a low current is injected, holes injected from the secondconductive type semiconductor layer 130 (for example, a hole injectionlayer) into the active layer are injected into the quantum well of thefirst active layer 121. Holes injected into the quantum well of thefirst active layer 121 are placed at a quantized energy level “n=1”having the lowest energy state. Holes placed at the quantized energylevel “n=1” are quantum-mechanically confined in a quantum well, andsince the holes have relatively high effective mass and low mobilitycompared to electrons, the holes do not pass through the gate quantumbarrier 125 and move to the second active layer 122. According to thisembodiment, the quantum well of the first active layer 121 may have athickness of about 2 nm to about 16 nm. According to this embodiment,the quantum well of the first active layer 121 may have a thickness ofabout 2 nm to about 10 nm. Electrons injected from the first conductivetype semiconductor layer 110 (for example, an electron injection layer)into the active layer 120 have low quantum-mechanical effective mass andhigh mobility compared to holes, and thus, the injected electrons mayeasily pass through the second active layer 122 and the gate quantumbarrier 125 and reach the quantum well of the first active layer 121.

Electrons injected into the quantum well of the first active layer 121are placed at the quantized energy level “n=1” having the lowest energystate. As a result, electrons and holes, which have been injected wheninjecting a low current, are combined in the quantum well of the firstactive layer 121 to emit light.

On the other hand, when a high current is injected, holes injected fromthe second conductive type semiconductor layer 130 (for example, a holeinjection layer) into the active layer 120 fill all quantized energylevels in the quantum wells of the first active layer 121, and then,surplus holes pass over the gate quantum barrier 125 and are injectedinto the second active layer 122. The second active layer 122 includes asuper lattice mini-band, and thus may quantum-mechanically accommodaterelatively more holes than the quantum well of the first active layer121, in the mini-band.

According to this embodiment, the second active layer 122 may have asuper lattice structure where a quantum well having a small energy bandgap and a quantum barrier having a large energy band gap are alternatelystacked at least two times or more, and the tunneling of electrons andholes may be performed quantum-mechanically. According to thisembodiment, the number of quantum wells in the first active layer 122may be about two to about twenty.

According to this embodiment, the size of the energy band gap of thequantum well in the first active layer 121 may be equal to or greaterthan that of the energy band gap of the quantum wells 122 a to 122 d.This is because holes pass over the gate quantum barrier 125 in thefirst active layer 121 and are effectively transported to the secondactive layer 122 when an injected current is equal to or greater than acertain value. Hole injection efficiency is fundamentally increased whenholes are injected from a position having a high energy state to aposition having a low energy state.

Holes injected into the second active layer 122 are effectivelydispersed into an entire super lattice, and are quantum-mechanicallycombined with electrons injected from the electron injection layer toemit light. As a result, electrons and holes, which have been injectedwhen injecting a high current, may be dispersed into the first andsecond active layers 121 and 122 and effectively combined therein toemit light.

According to this embodiment, the amount of injected current necessaryfor the operation of a device may not clearly be differentiated in a lowcurrent region and a high current region but variably selected andcontrolled according to usability of a light emitting device to beimplemented.

According to this embodiment, injection efficiency of holes injectedfrom the first active layer 121 into the second active layer 122 may beeffectively controlled according to the energy barrier height andthickness of the gate quantum barrier 125. According to this embodiment,furthermore, injection efficiency of holes injected from the firstactive layer 121 into the second active layer 122 may be effectivelyvaried by relatively controlling the size of the energy band gap in thefirst active layer 121 and the size of the energy band gap in the secondactive layer 122.

According to this embodiment, when the energy band gap of the firstactive layer 121 is equal to or greater than that of the second activelayer 122 in size, holes may be effectively transported from the firstactive layer 121 to the second active layer 122 at a certain injectioncurrent or higher.

FIG. 7 shows light emission efficiency characteristic based on theinjection current of a dual-active nitride semiconductor light emittingdevice according to a first embodiment. In manufacturing a device, athin film growth process uses Low-Pressure Metal-Organic Chemical VaporDeposition system (LPMOCVD), but the present disclosure is not limitedthereto. A sapphire substrate has been used as a substrate. Thesubstrate has been removed by applying a laser lift-off process, andthereafter, a vertical LED chip has been manufactured.

To compare effects, a related art blue light emitting device includingfive quantum well layers has been manufactured. According to FIG. 7, adual-active light emitting device according to the embodiment showsbetter light emission efficiency characteristics in all injectioncurrent regions than internal light emission efficiency of a related artnitride semiconductor blue light emitting device based on amultiple-quantum well structure.

According to the first embodiments, the light emitting device accordingto the first embodiment shows light efficiency that has been improvedfurther by at least 30% than the related art light emitting device, atan injection current of about 1000 mA.

<Second Embodiment>

FIG. 8 is a view schematically illustrating an energy band gap of anactive layer in a light emitting device (see the first structure)including a dual-active layer according to a second embodiment. In thesecond embodiment, a second active layer has a super lattice structure,and a first active layer has a multiple-quantum well structure includingtwo quantum well layers. The second embodiment may apply the technicalfeatures of the first embodiment.

A light emitting device 102 according to the second embodiment mayinclude a first active layer 121 having a multiple-quantum wellstructure, and thus may include a plurality of quantum wells 121 a and121 b, and a quantum barrier 121 c.

In the second embodiment, even when a current is injected in a lowcurrent region and an intermediate region, the first active layer 121may effectively operate as a main active layer compared to a case wherethe first active layer 121 has a multiple-quantum well structure and acase where the first active layer 121 includes a single quantum well.

For example, when a low current is injected, holes injected from thesecond conductive type semiconductor layer 130 (for example, a holeinjection layer) are confined in a first quantum well 121 a of the firstactive layer 121, and thereafter are combined with electrons to emitlight.

When a current is injected in the intermediate region, holes injectedfrom the hole injection layer fill quantized energy levels of the firstquantum well 121 a in the first active layer 121, and then, surplusholes pass over a quantum barrier 121 c in the first active layer 121,are injected into a second quantum well 121 b, and are combined withelectrons to emit light.

In the second embodiment, the number of quantum wells in the firstactive layer 121 may be about two to about three.

According to the second embodiment, in a case where the number ofquantum wells exceeds three in the multiple-quantum well structure ofthe first active layer 121, a relatively large serial resistance isgiven to holes, which are injected from the hole injection layer intothe second active layer 122 in injecting a high current, when theinjected holes pass through the first active layer 121 having themultiple-quantum well structure, and thus, hole injection efficiencytoward the second active layer 122 is decreased. Therefore, in a casewhere the number of quantum wells exceeds three in the multiple-quantumwell structure of the first active layer 121, the second active layer122 cannot effectively operate as a main active layer when injecting ahigh current.

In the second embodiment, the quantum barrier 121 c of the first activelayer 121 may be equal to or less than the thickness dg of the gatequantum barrier 125. In the second embodiment, for example, the quantumbarrier 121 c of the first active layer 121 may be about 0.2 nm to about7 nm.

According to the second embodiment, in a case where a thickness d1 ofthe quantum well 121 c in the first active layer 121 exceeds about 7 nm,holes, which are injected from the hole injection layer into the activelayer 120 in injecting an intermediate current and a high current, fillthe first quantum well 121 a of the first active layer 121, and then, ahigh serial resistance and nonradiative loss are given to surplus holeswhen the surplus holes pass through the relatively thick quantum barrier121 c, thereby decreasing hole injection efficiency toward the secondquantum well 121 b and the second active layer 122.

Therefore, when the thickness d1 of the quantum barrier 121 c in thefirst active layer 121 exceeds about 7 nm, the second quantum well 121 bof the first active layer 121 and the second active layer 122 may noteffectively participate in light emission in injecting an intermediatecurrent and a high current.

In the second embodiment, the thickness of the quantum well in the firstactive layer 121 may be about 2 nm to about 10 nm. According to thisembodiment, the size of an energy band gap of the quantum barrier 121 cin the first active layer 121 may be equal to or less than that of anenergy band gap of the gate quantum barrier 125. According to the secondembodiment, injection efficiency of holes, which are injected from thefirst active layer 121 into the second active layer 122 in increasing aninjected current, may be increased as the height of an energy barrier ofthe quantum barrier 121 c in the first active layer 121 becomes less andthe thickness of the energy barrier of the quantum barrier 121 c becomesless.

The intermediate current may be about 5 A/m2 or higher to about 35 A/m2or less. However, the present disclosure is not limited thereto.

Hereinafter, a method of manufacturing the light emitting deviceaccording to the first and second embodiments will be described.

For example, a first conductive type semiconductor layer 110, an activelayer 120 and a second conductive type semiconductor layer 130 areformed on a substrate (not shown) such as a sapphire substrate. Forexample, a nitride semiconductor electron injection layer is grown onthe substrate (not shown), and a nitride semiconductor active layer anda hole injection layer are grown and manufactured on the substrate.

A second active layer 122 including a super lattice structure may bemanufactured on a nitride semiconductor electron injection layer thinfilm, and a gate quantum barrier 125 may be manufactured between thesecond active layer 122 and the first active layer 121.

The super lattice structure of the second active layer 122 may bemanufactured by stacking a plurality of nitride semiconductor layershaving different energy band gaps. When the super lattice structure ofthe second active layer 122 may be manufactured by repeatedly stacking aplurality of nitride semiconductor layers having different energy bandgaps, the number of repeats may be at least two times or more. A nitridesemiconductor layer, having a large energy band gap in the super latticestructure of the second active layer 122, may have a thickness of about0.2 nm to about 7 nm, but the present disclosure is not limited thereto.

A nitride semiconductor layer, having a small energy band gap in thesuper lattice structure of the second active layer 122, may have athickness of about 2 nm to about 10 nm, but the present disclosure isnot limited thereto. The gate quantum barrier 125 between the secondactive layer 122 and the first active layer 121 may have a thickness ofabout 3 nm to about 15 nm, but the present disclosure is not limitedthereto.

Light emitted from the second active layer 122 and light emitted fromthe first active layer 121 may be manufactured to have an equal orsimilar wavelength. The number of quantum wells in the first activelayer 121 may be about one to about three. A quantum well layer of thefirst active layer 121 may have a thickness of about 2 nm to about 10nm, but the present disclosure is not limited thereto. When the firstactive layer 121 has a multiple-quantum well structure, a thickness d2of a quantum barrier may be manufactured as about 0.2 nm to about 7 nm,but the present disclosure is not limited thereto.

<Third Embodiment>

FIG. 9 is a view schematically illustrating an energy band gap (103) ofan active layer in a light emitting device (see the first epi structure)including a dual-active layer according to a third embodiment. In thethird embodiment, a second active layer 124 has a single quantum wellstructure having a relatively wide width, and a first active layer 121include a single quantum well structure having a relatively narrowwidth.

The third embodiment may apply the technical characteristics of thefirst and second embodiments.

In the light emitting structure according to the third embodiment, adual active layer includes the first active layer 121 having a narrowsingle quantum well that operates effectively in a low current region,the second active layer 124 having a wide single quantum well thatoperates effectively in a high current region, and a gate quantumbarrier 125 disposed between the first and second active layers 121 and124.

In the second embodiment, moreover, the first active layer 121 accordingto the third embodiment may include one or more quantum well layers.

According to the third embodiment, the first active layer 121 is formedrelatively thinner than the second active layer 124, and thus has betterquantum-mechanical quantum well confinement effect.

The thickness of the first active layer 121, disposed adjacently to thesecond conductive type semiconductor layer 130, may be about 1 nm toabout 10 nm. When the thickness of the first active layer 121 is lessthan about 1 nm, a sufficient amount of energy level may notquantum-mechanically be formed in an active layer (a light emissionlayer).

When the thickness of the first active layer 121 is greater than about10 nm, a quantum well confinement effect is relatively reducedquantum-mechanically. The first active layer 121 can provide excellentlight emission efficiency due to a quantum confinement effect wheninjecting a low current. According to this embodiment, the second activelayer 124 may have a thickness of about 3 nm to about 300 nm. When thethickness of the second active later 124 is about 300 nm or more, anonradiative loss effect due to a crystal defect is considerablyincreased, and thus the light emission efficiency of a light emittingdevice is largely decreased. In a case where the thickness of the secondactive layer 124 is less than about 3 nm, if a number of carriers areinjected, the second active layer 124 cannot effectively accommodate thecarriers, and thus, the light emission efficiency of a device isdecreased.

According to the third embodiment, the first active layer 121 isrelatively thinner than the second active layer 124. According to thethird embodiment, the second active layer 124 that is disposedadjacently to a first conductive type semiconductor layer 110 being anelectron injection layer enables N-type doping. For example, electronsthat are injected into the second active layer 124 doped in an N typemay pass through the second active layer 124 and be effectively injectedinto the first active layer 121.

In the light emitting device according to this embodiment, the firstactive layer 121 may act as a main active layer when a low current isinjected, and the second active layer 124 may act as a main active layerwhen a high current is injected.

According to the third embodiment, the size of the energy band gap ofthe second active layer 124, disposed near the first conductive typesemiconductor layer 110 being an N-type semiconductor layer, may beequal to or less than that of the energy band gap of the first activelayer 121 which is disposed near the second conductive typesemiconductor layer 130 being a P-type semiconductor layer.

According to this embodiment, when a low current is injected into thelight emitting device, holes may be sufficiently filled and thenconfined in the first active layer 121 having a low quantized energylevel, allow light to be emitted from the first active layer 121, andthereafter move to the second active layer 124. In this case, the gatequantum barrier 125 may be disposed between the second active layer 124and the first active layer 121, and formed to a thickness of about 3 nmto about 8 nm.

According to the third embodiment, the first active layer 121 isdescribed as one, but may be formed as two or more. FIG. 10 is a viewshowing optical output power characteristic based on the injectioncurrent of a dual-active nitride semiconductor blue light emittingdevice according to the third embodiment.

According to the third embodiment, FIG. 10 shows that the first activelayer including a narrow quantum well operates in the low current regionand the second active layer including a wide quantum well mainlyoperates in the high current region.

<Fourth Embodiment>

FIG. 11 is a view schematically illustrating an energy band gap (104) ofa nitride semiconductor light emitting device including a dual activelayer which includes a third active layer of a multiple-quantum wellstructure and a fourth active layer of a wide single quantum wellstructure, in a light emitting device according to a fourth embodiment.

The fourth embodiment may apply the technical characteristics of thefirst to third embodiments.

According to the fourth embodiment, a third active layer 123 adjacent toa first conductive type semiconductor layer 110 being an electroninjection layer may have a multiple-quantum well structure, and a fourthactive layer 126 adjacent to a second conductive type semiconductorlayer 120 being a hole injection layer may have a wide single quantumwell structure.

Each quantum well in the third active layer 123 may have a thickness ofabout 1 nm to about 10 nm, and the third active layer 123 may have athickness of about 3 nm to about 300 nm. According to the fourthembodiment, the thickness of the fourth active layer 126 may be greaterthan that of each quantum well in the third active layer 123.

According to the fourth embodiment, the fourth active layer 126 may beP-doped. According to the fourth embodiment, the size of an energy bandgap of the fourth active layer 126 having the wide well structure may beequal to or greater than that of an energy band gap of the quantum wellin the third active layer 123.

When a low current is injected into the light emitting device, thefourth active layer 126 may have a relatively large energy band gap. Forexample, since the fourth active layer 126 has been P-doped, holes maypass through the fourth active layer 126 and be injected into the thirdactive layer 123. Furthermore, electrons injected from the firstconductive type semiconductor layer 110 are combined with the holes toemit light, in the third active layer 123.

According to the fourth embodiment, the size of the energy band gap ofthe fourth active layer 126 adjacent to the second conductive typesemiconductor layer 130 being a hole injection layer may be equal to orgreater than that of the energy band gap of the first conductive typesemiconductor layer 110 being an electron injection layer, in terms ofhole injection efficiency.

Herein, a difference between the first epi structure (see the first tothird embodiments) and the structure according to the fourth embodimentis that the fourth active layer 126 adjacent to a P-type conductive typesemiconductor layer includes a wide well, namely, a well for a highcurrent, and thus, when the size of the energy band gap of the thirdactive layer 123 is the same as that of the energy band gap of thefourth active layer 126, since the fourth active layer 126 is relativelythicker, an energy level quantized in a thicker quantum well may have anenergy state quantum-mechanically lower than that of a ground state(n=1) energy level in the third active layer 123 which is relativelythinner.

Therefore, the thick fourth active layer 126 adjacent to a P-typeconductive type semiconductor layer may have an energy band gap greaterthan that of the third active layer 123 even a little, in regard to thesame mechanism as that of the first epi structure, namely, in regard tothe increase in hole injection efficiency.

Moreover, unlike the first epi structure, the fourth active layer 126 isadjacent to the P-type conductive type semiconductor layer 130 in thesecond epi structure (see the fourth embodiment). Accordingly, when alow current is injected, holes should be injected to the third activelayer 123 to primarily emit light, and thus unlike the first epistructure, the gate quantum barrier 125 may be designed relativelyfurther thinly such that tunneling is effectively performed wheninjecting a low current, in the second epi structure.

According to the fourth embodiment, as shown in FIG. 12, when a lowcurrent is injected into the light emitting device, electrons injectedfrom the first conductive type semiconductor layer 110 are mainlyconfined in the third active layer 123, but an electronic concentrationis relatively reduced in the fourth active layer 126.

FIG. 12 is a view showing a distribution of electrons and holes inside adual-active layer when a low current is injected into a light emittingdevice including the dual-active layer, according to a fourthembodiment.

When a high current is injected into the light emitting device, some ofelectrons injected from the first conductive type semiconductor layer110 into the active layer fill all quantized energy levels in themultiple-quantum well of the third active layer 123, and surpluselectrons pass over the gate quantum barrier 125 and are injected intothe fourth active layer 126 through tunneling or a drift transportprocess.

According to the fourth embodiment, as shown in FIG. 13, when a highcurrent is injected into the light emitting device, an electronconcentration is relatively increased in the fourth active layer 126 ina case of electrons injected from the first conductive typesemiconductor layer 110.

FIG. 13 is a view showing a distribution of electrons and holes inside adual-active layer when a high current is injected into a light emittingdevice including the dual-active layer, according to a fourthembodiment.

That is, as shown in FIG. 12, when a low current is injected into thelight emitting device, light is mainly emitted from the third activelayer 123 because an electron concentration is reduced in the fourthactive layer 126. However, as shown in FIG. 13, when a high current isinjected, light is conformally emitted from the third and fourth activelayers 123 and 126.

The fourth active layer 126 is thicker than the multiple-quantum well ofthe third active layer 123 and thus can effectively accommodate a lot ofelectrons, which are combined with holes to emit light.

According to the fourth embodiment, therefore, electrons and holes,which have been injected into the active layer when injecting a highcurrent, may be dispersed into the third and fourth active layers 123and 126 and effectively combined therein to emit light, therebyproviding high light emission efficiency in a high injection currentregion.

FIG. 14 is a view showing internal light emission quantum efficiencybased on an injected current density of a nitride semiconductor bluelight emitting device having a dual-active layer structure, according toa fourth embodiment. Comparing a light emitting device including only afirst active layer MQWs of a multiple-quantum well structure with alight emitting device including only a second active layer DH of a widesingle quantum well structure, as shown in FIG. 14, the dual-activelight emitting device according to the fourth embodiment relativelyprovides excellent internal quantum efficiency IQE in a wide injectioncurrent region.

(Fifth Embodiment)

FIG. 15 is a view schematically illustrating an energy band gap (105) ofan active layer of a light emitting device including a multiple activelayer, in a light emitting device according to a fifth embodiment.

For example, FIG. 15 is a view schematically illustrating an energy bandgap of an active layer of a multiple-active light emitting device whereone third active layer 124 has a multiple-quantum well structure (124 a,124 b), a fourth active layer 126 adjacent to a hole injection layer hasa wide single quantum well structure, and a fifth active 128 adjacent toan electron injection layer has the wide single quantum well structure,according to the third epi structure.

The fifth embodiment may apply the technical characteristics of thefourth embodiment.

In the fifth embodiment, the third active layer 124 having themultiple-quantum well structure is disposed between the fourth and fifthactive layers 126 and 128 having the wide single quantum well structure.

In a light emitting device according to the fifth embodiment, the thirdactive layer 124 having the multiple-quantum well structure disposed ata central portion of a multiple active layer mainly participates inlight emission, in a low current region, but the fourth and fifth activelayers 126 and 128 having the wide single quantum well structureparticipate in light emission mainly and effectively, in a high currentregion.

In the fifth embodiment, the gate quantum barrier is disposed betweenthe third and fourth active layers and between the third and fifthactive layers as in the embodiments.

In the light emitting device according to the fifth embodiment, a lightemitting mechanism in injecting a current operates similarly to thelight emitting mechanism that have been described above in theembodiments. The operating mechanism of the light emitting deviceaccording to the fifth embodiment will be described below in more detailwith reference to FIG. 15.

When a low current is injected, holes injected from the hole injectionlayer into the active layer pass through the fourth active layer 126,pass over a first gate quantum well barrier 125 a, and are injected intoa quantum well layer of the third active layer 124.

According to the fifth embodiment, when the size of an energy band gapof the fourth active layer 126 is greater than that of an energy bandgap of the quantum well layer in the third active layer 124, holeinjection efficiency can be increased.

When a low current is injected, electrons injected from the electroninjection layer into the active layer pass through the fifth activelayer 128, pass over a second gate quantum well barrier 125 b, and areinjected into the quantum well layer of the third active layer 124.

According to the fifth embodiment, when the size of an energy band gapof the fifth active layer 128 is greater than that of the energy bandgap of the quantum well layer in the third active layer 124, electroninjection efficiency can be increased.

As a result, when injecting a low current, electrons and holes areinjected into the third active layer 124 disposed at a central portionof the multiple active layer, and combined to emit light, effectively.

When a high current is injected, electrons injected from the electroninjection layer into the active layer fill all quantized energy levelsin the third active layer 124 disposed at a central portion, and surplusholes pass over the gate quantum barrier 125 a and 125 b and areeffectively injected to the fourth active layer 126 adjacent to the holeinjection layer and the fifth active layer 128 adjacent to the electroninjection layer.

Therefore, when injecting a high current, the fourth and fifth activelayers 126 and 128 mainly participate in light emission by effectivelyaccommodating a number of carriers.

FIG. 16 shows an optical output power for an injected current of anitride semiconductor blue light emitting device including a multipleactive layer, according to a fifth embodiment. FIG. 16 shows that thelight emission efficiency of the multiple active layer according to thefifth embodiment is far better than the optical output power of therelated art nitride semiconductor blue light emitting device including asingle active layer of a multiple-quantum well structure.

FIG. 17 is a cross sectional view illustrating a light emitting devicepackage according to an embodiment.

Referring to FIG. 17, a light emitting device package 200 according toan embodiment includes a package body 205, third and fourth electrodelayers 213 and 214 disposed in the package body 205, a light emittingdevice 100 that is disposed in the package body 205 and electricallyconnected to the third and fourth electrode layers 213 and 214, and amolding member 240 surrounding the light emitting device 100.

The package body 205 may be formed of a silicon material, a syntheticresin material, or a metal material. An inclined plane may be formedaround the light emitting device 100.

The third electrode layer 213 and the fourth electrode layer 214 areelectrically separated from each other and supply a power to the lightemitting device 100. Also, the third electrode layer 213 and the fourthelectrode layer 214 may reflect light emitted from the light emittingdevice 100 and thus improve light efficiency, and may dissipate heatgenerated by the light emitting device 100 to the outside.

The light emitting device according to the embodiments may be applied asthe light emitting device 100, but the present disclosure is not limitedthereto. The light emitting device 100 may apply a horizontal lightemitting device, a flip-chip light emitting device, or the like.

The light emitting device 100 may be disposed in the package body 205 oron the third electrode layer 213 or the fourth electrode layer 214.

The light emitting device 100 may be electrically connected to the thirdelectrode layer 213 and/or the fourth electrode layer 214 through a wire230. In the embodiment, the vertical light emitting device 100 using theone wire 230 is illustrated in the embodiment, but the presentdisclosure is not limited thereto.

The molding member 240 may surround the light emitting device 100,thereby protecting the light emitting device 100. The molding member 240may include a phosphor to vary a wavelength of light emitted form thelight emitting device 100.

The light emitting device 100 according to an embodiment may be appliedto a lighting system. The lighting system may include a lighting unitillustrated in FIG. 18, and a backlight unit illustrated in FIG. 19. Thelighting system may include a traffic light, a head light of a vehicle,a sign board, or the like.

FIG. 18 is a perspective view illustrating a lighting unit 1100according to an embodiment.

Referring to FIG. 18, the lighting unit 1100 may include a case body1110, a light emitting module 1130 disposed in the case body 1110, and aconnection terminal 1120 disposed in the case body 1120 to receive apower from an external power source.

The case body 1110 may be formed of a material having good heatdissipation characteristic. For example, the case body 1210 may beformed of a metal material or resin material.

The light emitting module 1130 may include a substrate 1132 and at leastone light emitting device package 200 mounted on the substrate 1132.

The substrate 1132 may be formed by printing a circuit pattern on aninsulating material. For example, the substrate 1132 may include aprinted circuit board (PCB), a metal core PCB, a flexible PCB, or aceramic PCB.

Also, the substrate 1132 may be formed of a material that efficientlyreflects light, or a surface of the substrate 1132 may be coated incolor (for example, white or silver color) that efficiently reflectslight.

At least one light emitting device package 200 may be mounted on thesubstrate 1132. Each light emitting device package 200 may include atleast one light emitting diode (LED) 100. The LED 100 may include acolored light emitting device that emits colored light such as red,green, blue, or white light, and an ultraviolet (UV) light emittingdevice that emits UV light.

As the light emitting device 100, the light emitting device according tothe embodiments may be applied.

The light emitting module 1130 may be disposed to have variouscombinations of the light emitting device package 200 in order to obtaincolor sense and brightness. For example, a white light emitting device,a red light emitting device, and a green light emitting device may bedisposed in combination with each other for securing a high colorrendering index (CRI).

The connection terminal 1120 is electrically connected to the lightemitting module 1130 to supply a power thereto. Referring to FIG. 18,the connection terminal 1120 is screwed into an external power source ina socket type, but the present disclosure is not limited thereto. Forexample, the connection terminal 1120 may be formed in a pin type andinserted into the external power source, or be connected to the externalpower source through a wire.

FIG. 19 is an exploded perspective view of a backlight unit 1200according to an embodiment.

The backlight unit 1200 according to an embodiment may include a lightguide plate 1210, a light emitting module 1240 supplying light to thelight guide plate 1210, a reflective member 1220 under the light guideplate 1210, and a bottom cover 1230 accommodating the light guide plate1210, light emitting module 1240 and reflective member 1220. However,the present disclosure is not limited thereto.

The light guide plate 1210 allows flat light to be supplied by diffusinglight. The light guide plate 1210 may be formed of a transparentmaterial, for example, may include one of acrylic resin such aspolymethyl metaacrylate (PMMA), polyethylene terephthalate (PET), polycarbonate (PC), and polyethylene naphthalate (PEN) resin.

The light emitting module 1240 supplies light to at least one side ofthe light guide plate 1210, namely, serves as a light source of adisplay device including the backlight unit 1200.

The light emitting module 1240 may contact the light guide plate 1210,but the present disclosure is not limited thereto. Specifically, thelight emitting module 1240 may include a substrate 1242 and a pluralityof light emitting device packages 200 mounted on the substrate 1242. Thesubstrate 1242 may contact the light guide plate 1210. However, thepresent disclosure is not limited thereto.

The substrate 1242 may be a PCB including a circuit pattern (not shown).The substrate 1242 may include a typical PCB, a metal core PCB, aflexible PCB, or the like, but the present disclosure is not limitedthereto.

The light emitting device packages 200 may be mounted on the substrate1242 such that a light emitting surface emitting light is separated by acertain distance from the light guide plate 1210.

The reflective member 1220 may be disposed under the light guide plate1210. The reflective sheet 1220 upwardly reflects light incident on abottom of the light guide plate 1210, thereby improving the brightnessof the backlight unit 1200. For example, the reflective member 1220 maybe formed of PET, PC, or PVS resin, but the present disclosure is notlimited thereto.

The bottom cover 1230 may receive the light guide plate 1210, the lightemitting module 1240, and the reflective member 1220. For this, thebottom cover 1230 may be formed in a box shape with opened top, but thepresent disclosure is not limited thereto.

The bottom cover 1230 may be formed of a metal material or a resinmaterial, and manufactured through a process such as press molding orextrusion molding. Embodiments provide the light emitting device, thelight emitting device package, and the lighting system, whichinnovatively solve nonradiative loss occurring in injecting a highcurrent and nonradiative loss due to a crystal defect occurring ininjecting a low current, which are the fundamental limitations of therelated art nitride semiconductor light emitting devices, therebyrealizing high efficient light emission characteristics in all injectioncurrent regions.

According to the embodiments, fields for applying the nitridesemiconductor light emitting device can be considerably increased.

According to the embodiments, the present disclosure can contribute tothe development of smart lighting products where an operating injectioncurrent varies in regions ranging from the low current region to thehigh current region.

Any reference in this specification to “one embodiment,” “anembodiment,” “example embodiment,” etc., means that a particularfeature, structure, or characteristic described in connection with theembodiment is included in at least one embodiment of the invention. Theappearances of such phrases in various places in the specification arenot necessarily all referring to the same embodiment. Further, when aparticular feature, structure, or characteristic is described inconnection with any embodiment, it is submitted that it is within thepurview of one skilled in the art to effect such feature, structure, orcharacteristic in connection with other ones of the embodiments.

Although embodiments have been described with reference to a number ofillustrative embodiments thereof, it should be understood that numerousother modifications and embodiments can be devised by those skilled inthe art that will fall within the spirit and scope of the principles ofthis disclosure. More particularly, various variations and modificationsare possible in the component parts and/or arrangements of the subjectcombination arrangement within the scope of the disclosure, the drawingsand the appended claims. In addition to variations and modifications inthe component parts and/or arrangements, alternative uses will also beapparent to those skilled in the art.

What is claimed is:
 1. A light emitting device, comprising: a firstconductive type semiconductor layer; a second conductive typesemiconductor layer; an active layer between the first conductive typesemiconductor layer and the second conductive type semiconductor layer,wherein the active layer comprises a first active layer and a secondactive layer adjacent to the first active layer; and a gate quantumbarrier between the first active layer and the second active layer,wherein a quantum-mechanically quantized density of state of the secondactive layer is greater than that of the first active layer, andwherein, when a first level of current is applied, the gate quantumbarrier confines a hole, which is injected into the first active layerthrough the second conductive type semiconductor layer, preventingtransport to the second active layer, and when a second level of currentthat is higher than the first level of current is applied, the gatequantum barrier allows the hole, which is injected into the first activelayer through the second conductive type semiconductor layer, to bedrift-transported to the second active layer.
 2. The light emittingdevice according to claim 1, wherein at least one of a color or awavelength of light emitted from the first active layer and lightemitted from the second active layer is the same.
 3. The light emittingdevice according to claim 1, wherein the second active layer comprises asuper lattice structure, and the first active layer comprises a singlequantum well structure.
 4. The light emitting device according to claim1, wherein the second active layer comprises a multiple-quantum well anda multiple-quantum barrier structure, and a quantum barrier in thesecond active layer provides for quantum-mechanical tunneling of acarrier.
 5. The light emitting device according to claim 1, wherein thefirst conductive type semiconductor layer is an electron injectionlayer, the second conductive type semiconductor layer is a holeinjection layer, and a size of an energy band gap of the first activelayer is greater than or equal to an energy band gap of the secondactive layer.
 6. The light emitting device according to claim 1, whereinthe first level of current is less than or equal to about 5 A/cm², andthe second level of current is greater than or equal to about 35 A/cm².7. The light emitting device according to claim 1, wherein a size of anenergy band gap of the gate quantum barrier is greater than a size of anenergy band gap of a quantum well in the first active layer, and is lessthan or equal to a size of an energy band gap of the second conductivetype semiconductor layer.
 8. The light emitting device according toclaim 1, wherein the first active layer comprises a quantum wellstructure having a first width, and the second active layer comprises asingle quantum well structure having a second width, the first widthbeing narrower than the second width.
 9. The light emitting deviceaccording to claim 8, wherein a thickness of the first active layer isabout 1 nm to about 10 nm, and a thickness of the second active layer isabout 3 nm to about 300 nm.
 10. The light emitting device according toclaim 8, wherein the first conductive type semiconductor layer is anelectron injection layer, the second conductive type semiconductor layeris a hole injection layer, and a size of an energy band gap of thesecond active layer is greater than or equal to a size of an energy bandgap of the first active layer.
 11. A light emitting device, comprising:a first conductive type semiconductor layer; a second conductive typesemiconductor layer; an active layer between the first conductive typesemiconductor layer and the second conductive type semiconductor layerwherein the active layer comprises a first active layer having amultiple-quantum well structure and a second active layer adjacent tothe first active layer and having a single quantum well structure; and agate quantum barrier between the first and second active layers, whereina quantum-mechanically quantized density of state of the first activelayer is greater than that of the second active layer, and wherein, whena first level of current is applied, the gate quantum barrier confines ahole, which is injected into the first active layer through the secondconductive type semiconductor layer, preventing transport to the secondactive layer, and when a second level of current that is higher than thefirst level of current is applied, the gate quantum barrier allows thehole, which is injected into the first active layer through the secondconductive type semiconductor layer, to be drift-transported to thesecond active layer.
 12. The light emitting device according to claim11, wherein the first conductive type semiconductor layer is an electroninjection layer, the second conductive type semiconductor layer is ahole injection layer, and a size of an energy band gap of the secondactive layer is greater than a size of an energy band gap of the firstactive layer.
 13. The light emitting device according to claim 11,wherein the first active layer comprises a quantum well structure havinga first width, and the second active layer comprises a single quantumwell structure having a second width, the first width being less thanthe second width.
 14. The light emitting device according to claim 11,further comprising a third active layer disposed between the firstconductive type semiconductor layer and the first active layer.
 15. Thelight emitting device according to claim 14, wherein at least one of acolor or a wavelength of light emitted from the third active layer orlight emitted from a fourth active layer is the same.
 16. The lightemitting device according to claim 15, wherein at least one of the thirdactive layer or the fourth active layer comprises a super latticestructure.
 17. The light emitting device according to claim 14, whereina quantum barrier of the third active layer is thinner than the gatequantum barrier.
 18. The light emitting device according to claim 14,wherein the active layer comprises a well and a barrier, and a width ofthe gate quantum barrier is greater than a width of the barrier.
 19. Thelight emitting device according to claim 14, wherein the first activelayer comprises a first well and a first barrier, wherein the secondactive layer comprises a second well and a second barrier, and wherein adepth of the first well is substantially same with a depth of the secondwell.